|Publication number||US7544955 B2|
|Application number||US 11/630,993|
|Publication date||Jun 9, 2009|
|Filing date||Jun 29, 2005|
|Priority date||Jul 1, 2004|
|Also published as||DE602005007899D1, EP1761756A1, EP1761756B1, US20080290294, WO2006005880A1|
|Publication number||11630993, 630993, PCT/2005/50515, PCT/FR/2005/050515, PCT/FR/2005/50515, PCT/FR/5/050515, PCT/FR/5/50515, PCT/FR2005/050515, PCT/FR2005/50515, PCT/FR2005050515, PCT/FR200550515, PCT/FR5/050515, PCT/FR5/50515, PCT/FR5050515, PCT/FR550515, US 7544955 B2, US 7544955B2, US-B2-7544955, US7544955 B2, US7544955B2|
|Original Assignee||Commissariat A L'energie Atomique|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (9), Non-Patent Citations (8), Referenced by (4), Classifications (6), Legal Events (2)|
|External Links: USPTO, USPTO Assignment, Espacenet|
The invention concerns techniques for measuring fluorescence in small quantities of liquid, and particularly in droplets of liquid.
Measuring fluorescence consists in exciting fluorescent markers in a liquid, by means of a light source of a predetermined wavelength.
The signal re-emitted by the markers is measured at another wavelength (higher than the excitation wavelength) by means of a detector.
A difficulty arises when one seeks to measure very low concentrations of markers. These fluorescent markers may be either fluorescent molecules, or quantum dots.
In this case, one has to detect a small quantity of fluoropohores in an often considerable background noise stemming, for example, from the fluorescence of the support of the sample measured, or dust or surrounding optical means, such as the optics of a microscope for example.
As illustrated in
The output voltage of the amplifier 8 is of the type:
G=gain of the amplifier
S=physical variable measured
Thus, the filter 8 is going to enable the useful signal to be recovered and the presence of noise b(t) to be minimised.
Since the phenomenon studied generally has slow variations, it therefore involves, most of the time, a low pass filtering.
The filtering may be obtained electronically or by integrating the signal over a certain period (case of CCD sensors) or even by averaging over several images.
The limitation of this type of device is that it does not enable low frequency noise to be eliminated such as, for example, the fluorescence of the substrate, the optics of any microscope, optical filters or even slow thermal fluctuations of the experiment.
One may do with this type of measurement if the signal to noise ratio corresponds to the requirements definition.
If this is not the case, a means of minimising the influence of low frequency noise has to be found.
It is sometimes possible to attenuate the effect of this noise by carrying out differential measurements compared to a negative control, but such a device has a certain number of disadvantages.
Firstly, it imposes size constraints since it is necessary to add a negative control and a supplementary sensor.
It also imposes cost constraints, because the device is more bulky and it therefore necessitates a longer development.
Finally, precision is not always assured because it is not certain that the negative control is exactly under the same thermal or chemical conditions as the positive control.
Synchronous detection enables a signal in a considerable noise to be measured without using negative control or supplementary sensor.
As illustrated in
Carrying out a synchronous detection measurement consists in varying periodically the physical phenomenon studied, in such a way as to modulate the physical variable measured.
With the modulation, the output signal of the amplifier 6 becomes:
Vout=G×S×cos(W m t)+b(t)
G=gain of the amplifier,
S=physical variable measured,
Wm=modulation pulsation (wm=2πfm),
The choice of the modulation frequency Wm is linked to the frequency zone where the spectral density of the noise is minimal.
The role of the selective filter 12 is going to consist in only conserving at the chain output the modulation frequency fm.
After amplification, by the amplifier 6, the signal is again multiplied by the multiplier 10 by the carrier cos(wmt)
V mult=(G×S×cos(w m t)+b(t))×cos(w m t)
V mult =G×S/2+(G×S/2)×cos(2w m t)+b(t)×cos(w m t).
The first component (GS/2) is continuous, the second is in 2wm and the third corresponds to the noise and is centered in wm.
After the multiplication, the signal is then filtered by a low pass integrator 12 to only conserve the component proportional to the signal of the sensor: G×S/2.
“Classical” synchronous detection is based for example on the modulation of the supply of the sensor or the light source. But it does not enable the fluorescence of the support or the optics to be eliminated because this fluorescence is also modulated.
Practically, the problem is therefore posed of finding a device and a method enabling a synchronous detection to be carried out on droplets or microdroplets of liquid.
Another problem is eliminating, in such a synchronous detection, any parasite fluorescence, while only conserving the signal coming from the droplet.
Preferably, such a method and such devices should enable various types of measurements to be carried out, such as fluorescence or spectrometry (especially absorption) or colorimetry measurements.
The invention concerns a method for producing a modulated optical signal from a droplet of a liquid medium comprising:
According to the invention, one uses a method of electrowetting to modulate the shape of the droplet at a defined frequency in order to carry out a synchronous detection of the light signal coming from the droplet and, in particular, to eliminate the background noise.
For example, within the scope of a laboratory on a chip, when the droplet, after a displacement, arrives on the detection zone, one or several electrodes may be activated to modify the shape of the droplet, then deactivated to make it recover its initial form, then activated again and so on.
The shape of the droplet varies therefore periodically over time, as does consequently the profile that the signal presents in the detector.
This detector measures a periodic signal and an instrumentation chain, or means of processing the signal, can analyze the signal coming from this synchronous detection on the measured signal.
The signal from the sensor can therefore be modulated to carry out a synchronous detection of the fluorescence or the absorption or any other optical phenomenon.
The modulation of the droplet may be achieved by means of a two-dimensional matrix or a row of electrodes of identical size.
In this case, it is the activation and the deactivation of the electrodes near to the droplet that modulates the shape of the droplet.
According to another possibility, the modulation may be obtained by a single electrode activated then deactivated, for example an electrode of lengthened shape.
The droplet may also be displaced in front of, then outside, the measurement window. Thus, the detection window receives either the fluorescence of the droplet when this is in front of the window, or the fluorescence of the background noise when the droplet is outside of the window.
This method of synchronous detection in the droplet may apply to any form of optical detection and, in particular, to a measurement in colorimetry, or in spectrometry, or in fluorescence.
The droplet may be confined, at least during its modulation, between the hydrophobic surface and an upper substrate.
The droplet may, before modulation, not be confined by the upper substrate. One is then in the case of a mixed system, which makes the droplet pass from a non confined state to a confined state.
It may also, before modulation, be confined by the upper substrate.
The invention further concerns a method of synchronous detection of an optical signal, comprising the implementation of a method as described above, then a step of demodulation of the optical signal.
The step of demodulation of the optical signal may comprise a multiplication of the modulated signal by a carrier signal at the frequency of modulation and a low pass filtering.
The invention further concerns a device for optically analyzing a droplet of a liquid medium comprising:
Such a device may further comprise a second substrate, arranged facing the hydrophobic surface.
This second substrate may further comprise a superficial hydrophobic layer and/or an electrode underneath.
The means for modulating the shape of a droplet, on the hydrophobic surface, by electrowetting, may comprise a plurality of electrodes under the hydrophobic surface.
These electrodes may be all of identical size, or instead one at least of the electrodes may be of lengthened shape.
A device for synchronous detection of an optical signal may comprise, apart from a device as described above, means carrying out a demodulation treatment of a synchronous signal.
A first embodiment of the invention, in open system, is illustrated in
This embodiment implements a device for displacing or manipulating droplets of liquid based on the principle of electrowetting on a dielectric.
Examples of such devices are described in the article of M. G. Pollack, A. D. Shendorov, R. B. Fair, entitled “Electro-wetting-based actuation of droplets for integrated microfluidics”, Lab Chip 2 (1) (2002) 96-101.
The forces used for the displacement of droplets of liquid are then electrostatic forces.
The document FR 2 841 063 also describes a device implementing, moreover, a catenary facing the activated electrodes for the displacement as counter electrode.
The principle of this type of displacement is summarized in
A droplet 2 is lying on a network 4 of electrodes, from which it is isolated by a dielectric layer 6 and a hydrophobic layer 8 (
The hydrophobic character of this layer signifies that the droplet has a contact angle, on this layer, greater than 90°.
The electrodes are themselves formed on the surface of a substrate 1.
When the electrode 4-1 located near to the droplet 2 is activated, by means of commutation means 14, the closing of which establishes a contact between this electrode and a voltage source 13 via a shared conductor 16, the dielectric layer 6 and the hydrophobic layer 8 between this activated electrode and the droplet, permanently polarized by a counter electrode 10, act as a capacitor. The effects of electrostatic charges induce the displacement of the droplet on the activated electrode. The counter electrode 10 enables the displacement by electrowetting, it maintains an electrical contact with the droplet during its displacement. This counter electrode 10 may be either a catenary as described in FR-2 841 063, or a buried wire, or a planar electrode on or in the cover of confined systems.
In open system, if there is no displacement, it is possible to spread out and modulate a droplet on the hydrophobic surface, without counter electrode. This is for example the case if the droplet may be brought onto the hydrophobic surface by a conventional dispensation system, the electrodes 4-1, 4-2 serving uniquely to spread out or to modulate the droplet at the spot where it has been deposited.
The droplet may thus be displaced if necessary step by step (
It is thereby possible to displace liquids, but also to mix them (by bringing droplets of different liquids together), and to carry out complex protocols.
The documents cited above give examples of implementations of series of adjacent electrodes for the manipulation of a droplet in a plane, the electrodes may indeed be arranged in a linear manner, but also in two dimensions, thereby defining a displacement plane for the droplets.
As illustrated in
Before activation of the electrodes, the droplet 2 lies on one of them; after activation of the electrodes 4-1, 4-2, 4-3, 4-4, the droplet 2 is stretched out and positioned above these four same electrodes.
The droplet is then in a state in which its length L (see
These same electrodes are then deactivated, which makes the droplet regain its initial shape, then again activated, then again deactivated and so on.
A beam 50, of wavelength suited to the desired measurement (with a view to a measurement of absorption or fluorescence or colorimetry or spectrometry) therefore sees its path in the droplet notably increased due to the lengthening of said droplet, then again reduced when said droplet recovers its initial shape, then again increased and so on.
The measurement signal is therefore modulated by modulation of the shape of the droplet itself. This is particularly advantageous when the volume of liquid examined is around, at the maximum, several microlitres, and can even attain very low values, for example around a nanolitre.
In a practical manner, one will position light emitting means 52, in such a way as to direct a beam 50 along the substrate.
A detector 54 will detect the modulated signal.
The activation of the electrodes 4 will make it possible, firstly if necessary to displace or position, then to modulate the shape of the droplet 2 along the beam 50, as explained above, and thereby to modulate the corresponding measured signal.
Therefore successions of activation—deactivation of the electrodes 4 are performed in order to modulate the signal as explained above.
The modulation may take place at a frequency between, for example, 10 Hz and 100 Hz.
In this figure, numerical references identical to those of
This device further comprises an upper substrate 100, preferably also covered with a hydrophobic layer 108. This assembly may if necessary be transparent, enabling an observation from above.
Here again, a light beam may be directed between the two substrates.
In a practical manner, one will position light emitting means, analogous to the means 52 of
The activation then the deactivation of the electrodes 4 of the lower substrate make it possible, firstly if necessary to displace or position, then to modulate the shape of the droplet 2 along the beam 50.
The catenary 10 of the previous figures is replaced, in this embodiment, by the electrode 112. The activation of this electrode and the repeated activation then the deactivation of the electrodes 4 makes it possible to displace the droplet 2 to the desired position then to modulate its shape as already explained above.
In the embodiments described above, several electrodes 4 are activated to deform and modulate the droplet. It is also possible to provide for an electrode of lengthened shape, the activation of which would enable the droplet to be flattened, again by electrowetting effect. The deactivation of this electrode would bring back the droplet to its initial shape. The droplet may then again be deformed and so on, thus achieving, once again, a modulation of the shape of the droplet in the path of the light beam 50, and thereby a modulation of the measured signal, whatever the nature of the measurement (absorption, fluorescence, transmission etc.).
The electrodes 4 receive an electric voltage, a voltage that may be amplified. The activation or the deactivation may take place via a relay or via an analogical, or digital, multiplexer, or a logic gate. The activation of the electrodes may be managed by computer or PC type digital means controlling relays such as the relays 14 of
Typically, the distance between any conductor 10 (
The conductor 10 is, for example, in the form of a wire of diameter between 10 μm and several hundreds of μm, for example 200 μm. This wire may be a wire of gold or aluminum or tungsten or other conductive materials.
When two substrates 1, 100 are used (
Whatever the embodiment considered, a droplet of liquid 2 will have a volume between, for example, 1 nanolitre and several microlitres, for example between 1 nl and 5 μl or 10 μl.
Moreover, each of the electrodes 4 will have for example a surface area of around several tens of μm2 (for example 10 μm2) up to 1 mm2, depending on the size of the droplets to be transported, the spacing between neighboring electrodes being for example between 1 μm and 10 μm.
The structuring of the electrodes 4 may be obtained by conventional microtechnology methods, for example by photolithography. The electrodes are for example formed by deposition of a metallic layer (Au, or Al, or ITO, or Pt, or Cr, or Cu, etc.) by photolithography. The substrate is then covered with a dielectric layer in SiN4, or SiO2, etc. Finally, a deposition of a hydrophobic layer is carried out such as, for example, a deposition of Teflon carried out by a spin coater.
Methods for forming chips incorporating a device according to the invention may be derived directly from the methods described in the document FR-2 841 063.
Conductors, and in particular buried conductors 112, may be formed by deposition of a conductive layer and etching of this layer following the appropriate pattern of conductors, before deposition of the hydrophobic layer 108.
The substrates 1, 100 are for example in silicon, or glass, or plastic.
Once a modulated signal conforming to the invention has been obtained, this signal may be amplified, multiplied by the modulation function at the frequency fm, function that is known, then integrated as already explained in liaison with
A device according to the invention may therefore comprise, moreover, means of synchronous detection: amplifier means 60, a multiplier 110, a low pass integrator 120 as illustrated in
The applied treatment will be that explained above in liaison with
The invention therefore concerns a method of synchronous detection of an optical signal, comprising the implementation of a method as described above, in order to acquire a modulated optical signal, then a step of demodulation of the optical signal.
The invention has in particular the following advantages:
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|International Classification||G01N21/01, G01J1/58, G01N1/00|
|Sep 5, 2008||AS||Assignment|
Owner name: COMMISSARIAT A L ENERGIE ATOMIQUE, FRANCE
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNOR:BOUTET, JEROME;REEL/FRAME:021487/0956
Effective date: 20061206
|Nov 20, 2012||FPAY||Fee payment|
Year of fee payment: 4